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THE JOURNEY THROUGH TIME

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MY'STORY

The MOVE Fire

This is a personal recollection on the Move fire on May 13, 1985 Philadelphia police fired thousands of rounds at the MOVE house, city officials approved dropping an explosive device on the roof, the resulting fire was allowed to burn, 11 people—including five children—died, and 61 homes were destroyed. Philadelphia City Council later called it a “brutal attack carried out by the City of Philadelphia on its own citizens” and acknowledged that no individual faced criminal consequences for the bombing. One timeline correction worth preserving for the BHP record: the major previous MOVE-police confrontation was August 8, 1978, about seven years before the bombing, not a year or two earlier. Officer James Ramp was killed, other police and firefighters were wounded, nine MOVE members were later convicted, and television cameras recorded police beating Delbert Africa during his arrest. The 1985 MOVE Commission later specifically criticized city planners for failing to adequately use lessons from that 1978 confrontation. And that actually strengthens the point you’re making: 1985 did not happen without precedent or institutional memory. There had already been a deadly confrontation with MOVE, years of conflict, negotiations and police involvement before Osage Avenue.

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BLACK FACTS
The Truths They Never Taught You...

The Violence That Helped Spark the NAACP

In August 1908, a white mob attacked Springfield, Illinois’s Black community, destroying homes and businesses and lynching two Black men. National outrage over the violence helped spur the movement that created the NAACP the following year.

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Wikipedia

Alternant matrix

In linear algebra, an alternant matrix is a matrix formed by applying a finite list of functions pointwise to a fixed column of inputs. An alternant determinant is the determinant of a square alternant matrix.

Generally, if are functions from a set to a field , and , then the alternant matrix has size and is defined by

or, more compactly, . (Some authors use the transpose of the above matrix.) Examples of alternant matrices include Vandermonde matrices, for which , and Moore matrices, for which .

Properties

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  • The alternant can be used to check the linear independence of the functions in function space. For example, let , and choose . Then the alternant is the matrix and the alternant determinant is . Therefore M is invertible and the vectors form a basis for their spanning set: in particular, and are linearly independent.
  • Linear dependence of the columns of an alternant does not imply that the functions are linearly dependent in function space. For example, let , and choose . Then the alternant is and the alternant determinant is 0, but we have already seen that and are linearly independent.
  • Despite this, the alternant can be used to find a linear dependence if it is already known that one exists. For example, we know from the theory of partial fractions that there are real numbers A and B for which . Choosing , , and , we obtain the alternant . Therefore, is in the nullspace of the matrix: that is, . Moving to the other side of the equation gives the partial fraction decomposition .
  • If and for any , then the alternant determinant is zero (as a row is repeated).
  • If and the functions are all polynomials, then divides the alternant determinant for all . In particular, if V is a Vandermonde matrix, then divides such polynomial alternant determinants. The ratio is therefore a polynomial in called the bialternant. The Schur polynomial is classically defined as the bialternant of the polynomials .

Applications

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See also

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References

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  • Muir, Thomas (2003) [1960]. A treatise on the theory of determinants. Dover Publications. pp. 321–363. ISBN 978-0-486-49553-8. OCLC 52203124.
  • Aitken, A.C. (1956). Determinants and Matrices (9th ed.). Oliver and Boyd Ltd. pp. 111–123. OCLC 271302373.
  • Stanley, Richard P. (1999). Enumerative Combinatorics (2nd ed.). Cambridge University Press. pp. 334–342. doi:10.1017/CBO9781139058520. ISBN 978-1-107-01542-5. OCLC 897778191.

Source: Wikipedia. Article content is retrieved live through the MediaWiki API.

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Wikipedia

Alternant matrix

In linear algebra, an alternant matrix is a matrix formed by applying a finite list of functions pointwise to a fixed column of inputs. An alternant determinant is the determinant of a square alternant matrix. Generally, if f 1 , f 2 , … , f n {\displaystyle f_{1},f_{2},\dots ,f_{n}} are functions from a set X {\displaystyle X} to a field F {\displaystyle F} , and α 1 , α 2 , … , α m ∈ X {\displaystyle {\alpha _{1},\alpha _{2},\ldots ,\alpha _{m}}\in X} , then the alternant matrix has size m × n {\displaystyle m\times n} and is defined by M = [ f 1 ( α 1 ) f 2 ( α 1 ) ⋯ f n ( α 1 ) f 1 ( α 2 ) f 2 ( α 2 ) ⋯ f n ( α 2 ) f 1 ( α 3 ) f 2 ( α 3 ) ⋯ f n ( α 3 ) ⋮ ⋮ ⋱ ⋮ f 1 ( α m ) f 2 ( α m ) ⋯ f n ( α m ) ] {\displaystyle M={\begin{bmatrix}f_{1}(\alpha _{1})&f_{2}(\alpha _{1})&\cdots &f_{n}(\alpha _{1})\\f_{1}(\alpha _{2})&f_{2}(\alpha _{2})&\cdots &f_{n}(\alpha _{2})\\f_{1}(\alpha _{3})&f_{2}(\alpha _{3})&\cdots &f_{n}(\alpha _{3})\\\vdots &\vdots &\ddots &\vdots \\f_{1}(\alpha _{m})&f_{2}(\alpha _{m})&\cdots &f_{n}(\alpha _{m})\\\end{bmatrix}}} or, more compactly, M i j = f j ( α i ) {\displaystyle M_{ij}=f_{j}(\alpha _{i})} . (Some authors use the transpose of the above matrix.) Examples of alternant matrices include Vandermonde matrices, for which f j ( α ) = α j − 1 {\displaystyle f_{j}(\alpha )=\alpha ^{j-1}} , and Moore matrices, for which f j ( α ) = α q j − 1 {\displaystyle f_{j}(\alpha )=\alpha ^{q^{j-1}}} .

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Wikipedia

Hermitian matrix

In mathematics, a Hermitian matrix (or self-adjoint matrix) is a square matrix with complex-valued entries that is equal to its own conjugate transpose. That is, if the element in the ⁠ j {\displaystyle j} ⁠-th row and ⁠ k {\displaystyle k} ⁠-th column of a Hermitian matrix ⁠ A {\displaystyle A} ⁠ is some complex number ⁠ A j k = x + i y {\displaystyle A_{jk}=x+iy} ⁠, then the element in the ⁠ k {\displaystyle k} ⁠-th row and ⁠ j {\displaystyle j} ⁠-th column is its complex conjugate ⁠ A k j = A j k ¯ = x − i y {\displaystyle A_{kj}={\overline {A_{jk}}}=x-iy} ⁠, for every pair of indices ⁠ j {\displaystyle j} ⁠ and ⁠ k {\displaystyle k} ⁠. Hermitian matrices can be understood as the complex generalization of symmetric real matrices. Using the notation ⁠ A T {\displaystyle \textstyle A^{\mathsf {T}}} ⁠ to mean the transpose of ⁠ A {\displaystyle A} ⁠ and an overline to mean the entrywise complex conjugate of a matrix, the Hermitian property is equivalent to the equality A = A T ¯ . {\displaystyle A={\overline {A^{\mathsf {T}}}}.} The conjugate transpose of a matrix is often denoted ⁠ A H {\displaystyle \textstyle A^{\mathsf {H}}} ⁠, in terms of which the Hermitian property can be more concisely expressed as ⁠ A = A H {\displaystyle \textstyle A=A^{\mathsf {H}}} ⁠. Equivalent notations in common use include ⁠ A H {\displaystyle \textstyle A^{\mathsf {H}}} ⁠, ⁠ A † {\displaystyle \textstyle A^{\dagger }} ⁠, and ⁠ A ∗ {\displaystyle \textstyle A^{*}} ⁠, although in quantum mechanics, A ∗ {\displaystyle \textstyle A^{*}} typically means the complex conjugate only, and not the conjugate transpose. Hermitian matrices are named after Charles Hermite, who demonstrated in 1855 that matrices of this form share with symmetric real matrices the property of always having real eigenvalues.

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Wikipedia

Vandermonde matrix

In linear algebra, a Vandermonde matrix, named after Alexandre-Théophile Vandermonde, is a matrix with the terms of a geometric progression in each row: an ( m + 1 ) × ( n + 1 ) {\displaystyle (m+1)\times (n+1)} matrix V = V ( x 0 , x 1 , ⋯ , x m ) = ( 1 x 0 x 0 2 … x 0 n 1 x 1 x 1 2 … x 1 n 1 x 2 x 2 2 … x 2 n ⋮ ⋮ ⋮ ⋱ ⋮ 1 x m x m 2 … x m n ) {\displaystyle V=V(x_{0},x_{1},\cdots ,x_{m})={\begin{pmatrix}1&x_{0}&x_{0}^{2}&\dots &x_{0}^{n}\\1&x_{1}&x_{1}^{2}&\dots &x_{1}^{n}\\1&x_{2}&x_{2}^{2}&\dots &x_{2}^{n}\\\vdots &\vdots &\vdots &\ddots &\vdots \\1&x_{m}&x_{m}^{2}&\dots &x_{m}^{n}\end{pmatrix}}} with entries V i , j = x i j {\displaystyle V_{i,j}=x_{i}^{j}} , the jth power of the number x i {\displaystyle x_{i}} , for all zero-based indices i {\displaystyle i} and j {\displaystyle j} . Some authors define the Vandermonde matrix as the transpose of the above matrix. The determinant of a square Vandermonde matrix (when n = m {\displaystyle n=m} ) is called a Vandermonde determinant or Vandermonde polynomial. Its value is: det ( V ) = ∏ 0 ≤ i < j ≤ n ( x j − x i ) = ( − 1 ) n ( n + 1 ) / 2 ∏ 0 ≤ i < j ≤ n ( x i − x j ) . {\displaystyle \det(V)=\prod _{0\leq i

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Moore matrix

In linear algebra, a Moore matrix, introduced by E. H. Moore (1896), is a matrix defined over a finite field. When it is a square matrix, its determinant is called a Moore determinant (this is unrelated to the Moore determinant of a quaternionic Hermitian matrix). The Moore matrix has successive powers of the Frobenius automorphism applied to its columns (beginning with the zeroth power of the Frobenius automorphism in the first column), so it is an m × n matrix M = [ α 1 α 1 q … α 1 q n − 1 α 2 α 2 q … α 2 q n − 1 α 3 α 3 q … α 3 q n − 1 ⋮ ⋮ ⋱ ⋮ α m α m q … α m q n − 1 ] {\displaystyle M={\begin{bmatrix}\alpha _{1}&\alpha _{1}^{q}&\dots &\alpha _{1}^{q^{n-1}}\\\alpha _{2}&\alpha _{2}^{q}&\dots &\alpha _{2}^{q^{n-1}}\\\alpha _{3}&\alpha _{3}^{q}&\dots &\alpha _{3}^{q^{n-1}}\\\vdots &\vdots &\ddots &\vdots \\\alpha _{m}&\alpha _{m}^{q}&\dots &\alpha _{m}^{q^{n-1}}\\\end{bmatrix}}} or M i , j = α i q j − 1 {\displaystyle M_{i,j}=\alpha _{i}^{q^{j-1}}} for all indices i and j. (Some authors use the transpose of the above matrix.) The Moore determinant of a square Moore matrix (so m = n) can be expressed as: det ( M ) = ∏ c ( c 1 α 1 + ⋯ + c n α n ) , {\displaystyle \det(M)=\prod _{\mathbf {c} }\left(c_{1}\alpha _{1}+\cdots +c_{n}\alpha _{n}\right),} where c runs over a complete set of direction vectors, made specific by having the last non-zero entry equal to 1, i.e., det ( M ) = ∏ 1 ≤ i ≤ n ∏ c 1 , … , c i − 1 ( c 1 α 1 + ⋯ + c i − 1 α i − 1 + α i ) . {\displaystyle \det(M)=\prod _{1\leq i\leq n}\prod _{c_{1},\dots ,c_{i-1}}\left(c_{1}\alpha _{1}+\cdots +c_{i-1}\alpha _{i-1}+\alpha _{i}\right).} In particular the Moore determinant vanishes if and only if the elements in the left hand column are linearly dependent over the finite field of order q. So it is analogous to the Wronskian of several functions. Dickson used the Moore determinant in finding the modular invariants of the general linear group over a finite field.

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TOPIC OF THE DAY

Greenwood / Black Wall Street

Before the 1921 destruction of Tulsa’s Greenwood District, Black residents had created a remarkable center of business and community life. The district included stores, professional offices, entertainment venues and homes owned by Black citizens. Understanding Greenwood means learning what was built—not only what was burned.

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TRIVIA QUESTION OF THE DAY

Which Black woman became the first elected to the United States Congress?

Shirley Chisholm, elected in 1968.